The stroboscopic surface of section we produced in the previous section is a Strange Attractor.
It is an attractor in the sense that trajectories
originating from various initial conditions converge
to it. It is Strange in the sense that it is neither
a continuous line in -
phase space (like a
Limit Cycle which forms a continuous trajectory
in phase space) nor is it filling the
-
plane.
It is a Fractal.
As in the case of the Driven One Well chaotic solution, this solution exhibits an extreme sensitivity to initial conditions. This is the hallmark of chaos.
This sensitivity to initial conditions and the
attractiveness of the Strange Attractor
can be illustrated
by following a bunch of trajectories based on
initial conditions that are fairly close together.
These trajectories should all converge to the
the Strange Attractor if observed in
a stroboscopic map at . Therefore they will
build the shape of the Strange Attractor
point by point. These points will be far apart
on the Strange Attractor due to the
exponential divergence of the orbits.
This Strange Attractor is really Strange!
Run the code for 1, 2, 3, 4, 5, 10, 20, 100 outside driving term periods ( via the option -t n ) thereby producing stroboscopic maps data to be plotted separately. This will illustrates divergence of the trajectories and the attraction of the Strange Attractor.
Michel Vallieres 2014-03-04